Variable Gap Tapering for LCLS-II Undulators

Size: px
Start display at page:

Download "Variable Gap Tapering for LCLS-II Undulators"

Transcription

1 Variable Gap Tapering for LCLS-II Undulators Heinz-Dieter Nuhn April 12, 2018 Continuous Taper, Apr 12,

2 Schematic Layout of LCLS-II New So; X- ray FEL with adjustable- gap undulator line (SXR) New Hard X- ray FEL with adjustable- gap undulator line (HXR) ~4.0 GeV kev gun- 2 gun- 1 Und. Hall SXR Dump sectors 0-10 SCRF Linac ~4 GeV Up to 1 MHz sectors Cu Linac GeV 120 Hz HXR kev kev 1-25 kev Continuous Taper, Apr 12,

3 LCLS-II SXR and HXR Component Layouts Cell Length: ± m Space for 2-stage HXRSS Location for upgraded HXRSS Space for SXRSS Cell Length: ± m Space for 3 Polarization Control Undulators Continuous Taper, Apr 12,

4 Undulator System Layout SXR Undulator Line HXR Undulator Line Continuous Taper, Apr 12,

5 LCLS-II SXR Undulator (HPU) Continuous Taper, Apr 12,

6 LCLS-II HXR Undulator (VPU) Continuous Taper, Apr 12,

7 LCLS-II Undulator Dimensions and Ranges Parameter SXU / SCRF SXU / Cu HXU / SCRF HXU / Cu Unit Undulator period length mm Total segment length m Number of periods per strong back X-ray energy range, required* kev Undulator operational gap range mm Undulator parameter range, K Electron energy range, operational GeV Maximum gap taper µm *at 4.0 GeV, the lower limit is 0.25 and 1.5 kev, respectively Continuous Taper, Apr 12,

8 LCLS Step Taper Only Continuous Taper, Apr 12,

9 LCLS-II Gap Encoder Difference [um] (Downstream Upstream) Continuous Taper, Apr 12,

10 LCLS-II Undulator Segment 300 µm taper over 3.4-m segment length (~88 µrad) Undulator Segment Strongbacks Upstream gap encoder Downstream gap encoder K/K ( g/ λ u ) g/ λ u Continuous Taper, Apr 12,

11 Large Taper Ranges at LCLS-II Continuous Taper, Apr 12,

12 SXU-007 Field Measurements: (1) Untapered <K pole > = ± K eff = ± Single Pole Hall Probe Data z 0 up,pole z 0 dn,pole K pole ( z pole )= Δ z pole /2π e/ m e c Δ z pole = z 0 dn,pole z 0 u z pole 1/2 ( z 0 dn,pole + z 0 Continuous Taper, Apr 12,

13 SXU-007 Field Measurements: (2) Tapered Measured K pole values for SXU tapers of +100 µm and +300 µm and reversed taper of -100 µm at 8 mm and 20 mm gap. Difference between tapered and untapered K pole values is only according to gap change. (No distortion at large tapers observed) Continuous Taper, Apr 12,

14 Field Evaluations for Tapered Undulators Standard calculations of phase shake and total phase assume constant beam energy and can not be applied to tapered undulators. Instead assume that taper is necessary because of energy loss along undulator segment, i.e., A value for can be found that minimizes the change of phase advance per period. α γ γ=γ(z)= γ start (1 α γ(z)= γ start f tp (z) f tp (z)={ 1&for z< z α γ ( z Continuous Taper, Apr 12,

15 Phase Calculations The phase slippage for changing energy along undulator segment is φ taper (z)= 2π/ λ u (1+ 1/2 K( g start ) 2 ) 0 z 1/ f tp ( z ) 2 (1+ The field integrals are calculated as usual I1x(z)= 0 z B x ( z )d z I1y(z)= 0 z B y ( z )d z The slopes and trajectories are d/dz y(z)= 1/ (Bρ) start d/dz I1x( z x(z)= 1/ (Bρ) start )/ f tp ( z ) I (Bρ) start = γ start m c/e y(z)= 1/ (Bρ) start 0 z I1x( z x(z)= 1/ (Bρ) start )/ f tp ( z ) 0 z d z Continuous Taper, Apr 12,

16 Phase Measurements φ taper (z)= 2π/ λ u (1+ 1/2 K( g start ) 2 ) 0 z 1/ f tp ( z ) 2 (1+ ( e/m c ) 2 ( I1x( z ) blue: untapered red: taper 300 µm, = α γ Difference During free space travel after undulator, phase advance per unit length is longer for larger regular tapers due to lower electron energies. ~360 degxray per period in both cases d/dz ( φ tapered φ untapered )= 360/ λ u (1+ 1/2 K( g start ) 2 ) ( 1/ For SXU-007, at 300 µm taper and 8 mm gap (1 α γ ) 2 1) d/dz ( φ tapered 38.6 degxray / m φ untapered )= Continuous Taper, Apr 12, 2018 This will be corrected with a phase shifter. 16

17 SXU-007 Trajectories BBA corrected horizontal and vertical trajectories for +300 µm SXU taper based on field measurements. Only insignificant deviation from untapered trajectories observed. Continuous Taper, Apr 12,

18 Summary The LCLS-II undulators allow continuous gap tapering Limits are ±300 µm over segment length (~±88 µrad) SXU taper measurements look promising: If adjusted to compensate for energy loss, tapering will mostly change the downstream phase advance will only slightly increase overall phase shake will not significantly steer the electron beam HXU (vertically polarizing undulator) taper measurements will follow soon Continuous Taper, Apr 12,

19 Thank you for your attention! Continuous Taper, Apr 12,

LCLS-II Undulator Tolerance Budget*

LCLS-II Undulator Tolerance Budget* LCLS-TN-13-5 rev2 April 16, 2013 LCLS-II Undulator Tolerance Budget* Heinz-Dieter Nuhn, Stanford Linear Accelerator Center, MS-18, 2575 Sandhill Road, Menlo Park, California 94025. 1 Introduction This

More information

LCLS Undulators Present Status and Future Upgrades

LCLS Undulators Present Status and Future Upgrades LCLS Undulators Present Status and Future Upgrades Heinz-Dieter Nuhn LCLS Undulator Group Leader 1 1 Heinz-Dieter Nuhn Linac Coherent Light Source INJECTOR LINAC BEAM TRANSPORT UNDULATOR HALL 2 2 Heinz-Dieter

More information

E ect Of Quadrant Taper On Delta Undulator Phase Errors

E ect Of Quadrant Taper On Delta Undulator Phase Errors LCLS-TN-5- E ect Of Quadrant Taper On Delta Undulator Phase Errors Zachary Wolf SLAC February 8, 05 Abstract The elds in the Delta undulator are very sensitive to the position of the magnet arrays. A taper

More information

Vertical Polarization Option for LCLS-II. Abstract

Vertical Polarization Option for LCLS-II. Abstract SLAC National Accelerator Lab LCLS-II TN-5-8 March 5 Vertical Polarization Option for LCLS-II G. Marcus, T. Raubenheimer SLAC, Menlo Park, CA 95 G. Penn LBNL, Berkeley, CA 97 Abstract Vertically polarized

More information

LCLS-II Capabilities & Overview LCLS-II Science Opportunities Workshop. Tor Raubenheimer (P. Emma) February 9 th, 2015

LCLS-II Capabilities & Overview LCLS-II Science Opportunities Workshop. Tor Raubenheimer (P. Emma) February 9 th, 2015 LCLS-II Capabilities & Overview LCLS-II Science Opportunities Workshop Tor Raubenheimer (P. Emma) February 9 th, 2015 Outline 1. Overall machine goals and layout 2. Primary parameters Nominal X-ray wavelength

More information

FEL SIMULATION AND PERFORMANCE STUDIES FOR LCLS-II

FEL SIMULATION AND PERFORMANCE STUDIES FOR LCLS-II FEL SIMULATION AND PERFORMANCE STUDIES FOR LCLS-II G. Marcus, Y. Ding, P. Emma, Z. Huang, T. Raubenheimer, L. Wang, J. Wu SLAC, Menlo Park, CA 9, USA Abstract The design and performance of the LCLS-II

More information

LCLS Undulator Parameter Workshop

LCLS Undulator Parameter Workshop LCLS Undulator Parameter Workshop Performance Analysis Using RON (and some notes on the LCLS prototype) Roger Dejus and Nikolai Vinokurov October 24, 2003 Budker Institute of Nuclear Physics, Novosibirsk

More information

A PPM Phase Shifter Design

A PPM Phase Shifter Design LCLS-TN-- A PPM Phase Shifter Design Zachary Wolf SLAC July 30, 0 Abstract This note describes the design of a pure permanent magnet (PPM) phase shifter for LCLS-II. A PPM phase shifter has the advantage

More information

X-Ray Diagnostics Commissioning at the LCLS

X-Ray Diagnostics Commissioning at the LCLS X-Ray Diagnostics Commissioning at the LCLS - Selected Studies - J. Welch, SLAC National Accelerator Laboratory Aug. 3-27, 2010 Commissioning Studies Microbunching Instability Laser Heater tune-up Gas

More information

Demonstration of Energy-Chirp Control in Relativistic Electron Bunches at LCLS Using a Corrugated Structure. Karl Bane, 7 April 2017,, KEK

Demonstration of Energy-Chirp Control in Relativistic Electron Bunches at LCLS Using a Corrugated Structure. Karl Bane, 7 April 2017,, KEK Demonstration of Energy-Chirp Control in Relativistic Electron Bunches at LCLS Using a Corrugated Structure Karl Bane, 7 April 2017,, KEK Introduction At the end of acceleration in an X-ray FEL, the beam

More information

LCLS Commissioning Status

LCLS Commissioning Status LCLS Commissioning Status Paul Emma (for the LCLS Commissioning Team) June 20, 2008 LCLS ANL LLNL UCLA FEL Principles Electrons slip behind EM wave by λ 1 per undulator period ( (λ u ) x K/γ e λ u v x

More information

LCLS-II SCRF start-to-end simulations and global optimization as of September Abstract

LCLS-II SCRF start-to-end simulations and global optimization as of September Abstract SLAC National Accelerator Lab LCLS-II TN-17-4 February 217 LCLS-II SCRF start-to-end simulations and global optimization as of September 216 G. Marcus SLAC, Menlo Park, CA 9425 J. Qiang LBNL, Berkeley,

More information

OPTIMIZATION OF COMPENSATION CHICANES IN THE LCLS-II BEAM DELIVERY SYSTEM

OPTIMIZATION OF COMPENSATION CHICANES IN THE LCLS-II BEAM DELIVERY SYSTEM OPTIMIZATION OF COMPENSATION CHICANES IN THE LCLS-II BEAM DELIVERY SYSTEM LCLS-II TN-15-41 11/23/2015 J. Qiang, M. Venturini November 23, 2015 LCLSII-TN-15-41 1 Introduction L C L S - I I T E C H N I C

More information

Coherent X-Ray Sources: Synchrotron, ERL, XFEL

Coherent X-Ray Sources: Synchrotron, ERL, XFEL Coherent X-Ray Sources: Synchrotron, ERL, XFEL John Arthur SSRL/SLAC Energy Recovery Linac Science Workshop Cornell University 2 December 2000 Supported by the US Dept. of Energy, Office of Basic Energy

More information

Undulator Field Integral Measurements

Undulator Field Integral Measurements LCLS-TN-05-22 Undulator Field Integral Measurements Zachary Wolf SLAC August 5, 2005 Abstract The LCLS undulator eld integrals must be very small so that the beam trajectory slope and o set stay within

More information

Undulator Commissioning Spectrometer for the European XFEL

Undulator Commissioning Spectrometer for the European XFEL Undulator Commissioning Spectrometer for the European XFEL FEL Beam Dynamics Group meeting DESY, Hamburg, Nov. 9 th 010 Wolfgang Freund, WP74 European XFEL wolfgang.freund@xfel.eu Contents Undulator commissioning

More information

Short Pulse, Low charge Operation of the LCLS. Josef Frisch for the LCLS Commissioning Team

Short Pulse, Low charge Operation of the LCLS. Josef Frisch for the LCLS Commissioning Team Short Pulse, Low charge Operation of the LCLS Josef Frisch for the LCLS Commissioning Team 1 Normal LCLS Parameters First Lasing in April 10, 2009 Beam to AMO experiment August 18 2009. Expect first user

More information

Status of X-ray FEL/SPring-8 Machine Construction

Status of X-ray FEL/SPring-8 Machine Construction T. Shintake@ Oct 2008 Status of X-ray FEL/SPring-8 Machine Construction Representing JASRI+RIKEN Joint Team T. Shintake RIKEN/SPring-8 Status of 8 GeV XFEL/SPring-8 Construction What we learned from SCSS

More information

Chromatic Corrections for the LCLS-II Electron Transport Lines

Chromatic Corrections for the LCLS-II Electron Transport Lines Chromatic Corrections for the LCLS-II Electron Transport Lines LCLS-II TN-16-07 3/4/2016 P. Emma, Y. Nosochkov, M. Woodley March 23, 2016 LCLSII-TN-16-07 Chromatic Corrections for the LCLS-II Electron

More information

Radiation Safety at LCLS: The Photon Beam s Maximum Capability and Material Damage Potential

Radiation Safety at LCLS: The Photon Beam s Maximum Capability and Material Damage Potential SLAC-PUB-15708 August 2013 Radiation Safety at LCLS: The Photon Beam s Maximum Capability and Material Damage Potential J.M. Bauer *1, J.C. Liu 1, A.A. Prinz 2, and S.H. Rokni 1 1 Radiation Protection

More information

Operational Performance of LCLS Beam Instrumentation. Henrik Loos, SLAC BIW 2010, Santa Fe, NM

Operational Performance of LCLS Beam Instrumentation. Henrik Loos, SLAC BIW 2010, Santa Fe, NM Editor's Note: PDF version of slides from Beam Instrumentation Workshop 21, Santa Fe, NM Operational Performance of LCLS Beam Instrumentation Henrik Loos, SLAC BIW 21, Santa Fe, NM BIW 21 1 1 Henrik Loos

More information

LOLA: Past, present and future operation

LOLA: Past, present and future operation LOLA: Past, present and future operation FLASH Seminar 1/2/29 Christopher Gerth, DESY 8/5/29 FLASH Seminar Christopher Gerth 1 Outline Past Present Future 8/5/29 FLASH Seminar Christopher Gerth 2 Past

More information

2.6 Electron transport lines

2.6 Electron transport lines 2.6 Electron transport lines 2.6 Electron transport lines Overview The electron transport lines consist of all of the electron beamline segments that are neither part of the Linacs nor part of the injector.

More information

The MID instrument.

The MID instrument. The MID instrument International Workshop on the Materials Imaging and Dynamics Instrument at the European XFEL Grenoble, Oct 28/29, 2009 Thomas Tschentscher thomas.tschentscher@xfel.eu Outline 2 History

More information

X-band RF driven hard X-ray FELs. Yipeng Sun ICFA Workshop on Future Light Sources March 5-9, 2012

X-band RF driven hard X-ray FELs. Yipeng Sun ICFA Workshop on Future Light Sources March 5-9, 2012 X-band RF driven hard X-ray FELs Yipeng Sun ICFA Workshop on Future Light Sources March 5-9, 2012 Motivations & Contents Motivations Develop more compact (hopefully cheaper) FEL drivers, L S C X-band (successful

More information

Alignment requirement for the SRF cavities of the LCLS-II injector LCLSII-TN /16/2014

Alignment requirement for the SRF cavities of the LCLS-II injector LCLSII-TN /16/2014 Alignment requirement for the SRF cavities of the LCLS-II injector LCLS-II TN-14-16 12/16/2014 R. K. Li, C. Papadopoulos, T. O. Raubenheimer, J. F. Schmerge, and F. Zhou December 16, 2014 LCLSII-TN-14-16

More information

LCLS-II Beam Stay-Clear

LCLS-II Beam Stay-Clear LCLSII-TN-14-15 LCLS-II Beam Stay-Clear J. Welch January 23, 2015 1 Introduction This note addresses the theory and details that go into the Beam Stay-Clear (BSC) requirements for LCLS-II [1]. At a minimum

More information

FIRST LASING OF THE LCLS X-RAY FEL AT 1.5 Å

FIRST LASING OF THE LCLS X-RAY FEL AT 1.5 Å FIRST LASING OF THE LCLS X-RAY FEL AT 1.5 Å P. Emma, for the LCLS Commissioning Team; SLAC, Stanford, CA 94309, USA Abstract The Linac Coherent Light Source (LCLS) is a SASE 1.5-15 Å x-ray Free-Electron

More information

Some Sample Calculations for the Far Field Harmonic Power and Angular Pattern in LCLS-1 and LCLS-2

Some Sample Calculations for the Far Field Harmonic Power and Angular Pattern in LCLS-1 and LCLS-2 Some Sample Calculations for the Far Field Harmonic Power and Angular Pattern in LCLS-1 and LCLS-2 W.M. Fawley February 2013 SLAC-PUB-15359 ABSTRACT Calculations with the GINGER FEL simulation code are

More information

Update on and the Issue of Circularly-Polarized On-Axis Harmonics

Update on and the Issue of Circularly-Polarized On-Axis Harmonics Update on FERMI@Elettra and the Issue of Circularly-Polarized On-Axis Harmonics W. Fawley for the FERMI Team Slides courtesy of S. Milton & Collaborators The FERMI@Elettra Project FERMI@Elettra is a single-pass

More information

Beam Pipe Corrector Study

Beam Pipe Corrector Study LCLS-TN-12-1 Beam Pipe Corrector Study Zachary Wolf, Yurii Levashov SLAC March 19, 2012 Abstract This note describes the test of a corrector magnet which can be built into the beam pipe of the LCLS-II

More information

Undulator Line Developments Update. Efim Gluskin APS/ANL LCLS TAC Meeting, SLAC, Stanford December 10-11, 2001

Undulator Line Developments Update. Efim Gluskin APS/ANL LCLS TAC Meeting, SLAC, Stanford December 10-11, 2001 Undulator Line Developments Update Efim Gluskin APS/ANL LCLS TAC Meeting, SLAC, Stanford December 10-11, 2001 Undulator Prototype Magnetic characterization of magnets Mechanical certification of poles

More information

Delta Undulator End Design

Delta Undulator End Design LCLS-TN-1- Delta Undulator End Design Zachary Wolf SLAC January 9, 01 Abstract This note describes the magnetic end design of the Delta undulator. Both three block ends and two block ends were studied.

More information

HARMONIC LASING OPTIONS FOR LCLS-II

HARMONIC LASING OPTIONS FOR LCLS-II MOP54 Proceedings of FEL4, Basel, Switzerland HARMONIC LASING OPTIONS FOR LCLS-II G. Marcus, Y. Ding, Z. Huang, T. Raubenheimer, SLAC, Menlo Park, CA 945, USA G. Penn, LBNL, Berkeley, CA 947, USA Copyright

More information

Undulator K Value Temperature Dependence

Undulator K Value Temperature Dependence LCLS-TN-09-4 Undulator K Value Temperature Dependence Zachary Wolf, Yurii Levashov SLAC October 6, 2009 Abstract LCLS undulator SN27 was used to measure the temperature dependence of its K value. The results

More information

II) Experimental Design

II) Experimental Design SLAC Experimental Advisory Committee --- September 12 th, 1997 II) Experimental Design Theory and simulations Great promise of significant scientific and technological achievements! How to realize this

More information

Ballistic Orbit at FLASH: Latest Results. P. Castro (MPY)

Ballistic Orbit at FLASH: Latest Results. P. Castro (MPY) Ballistic Orbit at FLASH: Latest Results P. Castro (MPY) Contents of this talk: What ballistic orbit is Our Motivation A little bit of history Last Results Outlook What ballistic orbit is: a beam trajectory

More information

Generation and characterization of ultra-short electron and x-ray x pulses

Generation and characterization of ultra-short electron and x-ray x pulses Generation and characterization of ultra-short electron and x-ray x pulses Zhirong Huang (SLAC) Compact XFEL workshop July 19-20, 2010, Shanghai, China Ultra-bright Promise of XFELs Ultra-fast LCLS Methods

More information

Femto-second FEL Generation with Very Low Charge at LCLS

Femto-second FEL Generation with Very Low Charge at LCLS Femto-second FEL Generation with Very Low Charge at LCLS Yuantao Ding, For the LCLS commissioning team X-ray Science at the Femtosecond to Attosecond Frontier workshop May 18-20, 2009, UCLA SLAC-PUB-13525;

More information

Check the LCLS Project website to verify 2 of 6 that this is the correct version prior to use.

Check the LCLS Project website to verify 2 of 6 that this is the correct version prior to use. 1. Introduction The XTOD Offset Systems are designed to spatially separate the useful FEL radiation from high-energy spontaneous radiation and Bremsstrahlung γ-rays. These unwanted radiations are generated

More information

A 6 GeV Compact X-ray FEL (CXFEL) Driven by an X-Band Linac

A 6 GeV Compact X-ray FEL (CXFEL) Driven by an X-Band Linac A 6 GeV Compact X-ray FEL (CXFEL) Driven by an X-Band Linac Zhirong Huang, Faya Wang, Karl Bane and Chris Adolphsen SLAC Compact X-Ray (1.5 Å) FEL Parameter symbol LCLS CXFEL unit Bunch Charge Q 250 250

More information

Wakefield Effects of Collimators in LCLS-II

Wakefield Effects of Collimators in LCLS-II Wakefield Effects of Collimators in LCLS-II LCLS-II TN-15-38 10/7/2015 K. Bane SLAC, Menlo Park, CA 94025, USA October 7, 2015 LCLSII-TN-15-38 L C L S - I I T E C H N I C A L N O T E LCLS-TN-15-38 October

More information

Two-Stage Chirped-Beam SASE-FEL for High Power Femtosecond X-Ray Pulse Generation

Two-Stage Chirped-Beam SASE-FEL for High Power Femtosecond X-Ray Pulse Generation Two-Stage Chirped-Beam SASE-FEL for High ower Femtosecond X-Ray ulse Generation C. Schroeder*, J. Arthur^,. Emma^, S. Reiche*, and C. ellegrini* ^ Stanford Linear Accelerator Center * UCLA 12-10-2001 LCLS-TAC

More information

WG2 on ERL light sources CHESS & LEPP

WG2 on ERL light sources CHESS & LEPP Charge: WG2 on ERL light sources Address and try to answer a list of critical questions for ERL light sources. Session leaders can approach each question by means of (a) (Very) short presentations (b)

More information

Introduction To LCLS Undulator Tuning

Introduction To LCLS Undulator Tuning LCLS-TN-04-7 Introduction To LCLS Undulator Tuning Zachary Wolf June 3, 2004 Abstract This note gives a general introduction to undulator tuning for the LCLS. It starts with a theoretical discussion in

More information

COMMISSIONING OF THE DELTA POLARIZING UNDULATOR AT LCLS*

COMMISSIONING OF THE DELTA POLARIZING UNDULATOR AT LCLS* COMMISSIONING OF THE DELTA POLARIZING UNDULATOR AT LCLS* H.-D. Nuhn #, S.D. Anderson, R.N. Coffee, Y. Ding, Z. Huang, M. Ilchen, Y. Levashov, A.A. Lutman, J. MacArthur, A. Marinelli, S.P. Moeller, F. Peters,

More information

LCLS Start-Up Test Plan

LCLS Start-Up Test Plan LCLS Physics Requirement Document #1.1-2 Project Management Revision 0 LCLS Start-Up Test Plan H-D. Nuhn Author Signature Date J. Welch Author Signature Date J. Galayda Project Director Signature Date

More information

Length of beam system = 910m. S. Reiche X var = ~50m ~ 650m / Y. Kim FEL-KY ~150m. ~60m. LaserHutch2 (access during operation)

Length of beam system = 910m. S. Reiche X var = ~50m ~ 650m / Y. Kim FEL-KY ~150m. ~60m. LaserHutch2 (access during operation) Laser Laser HHG Diagnostic ATHOS PORTHOS ARAMIS THz-Pump P A U L S C H E R R E R I N S T I T U T Length of beam system = 910m &'!( Test & Commissioning steps (A,B,C) A11 Conv. Gun & Injector A12 LINAC

More information

Electron Linear Accelerators & Free-Electron Lasers

Electron Linear Accelerators & Free-Electron Lasers Electron Linear Accelerators & Free-Electron Lasers Bryant Garcia Wednesday, July 13 2016. SASS Summer Seminar Bryant Garcia Linacs & FELs 1 of 24 Light Sources Why? Synchrotron Radiation discovered in

More information

X-ray Free-electron Lasers

X-ray Free-electron Lasers X-ray Free-electron Lasers Ultra-fast Dynamic Imaging of Matter II Ischia, Italy, 4/30-5/3/ 2009 Claudio Pellegrini UCLA Department of Physics and Astronomy Outline 1. Present status of X-ray free-electron

More information

Calculation Of Fields On The Beam Axis Of The Delta Undulator

Calculation Of Fields On The Beam Axis Of The Delta Undulator LCLS-TN-3- Calculation Of Fields On The Beam Axis Of The Delta Undulator Zachary Wolf SLAC April, 20 Abstract It is not possible to do Hall probe measurements on the beam axis of the Delta undulator since

More information

First operation of a Harmonic Lasing Self-Seeded FEL

First operation of a Harmonic Lasing Self-Seeded FEL First operation of a Harmonic Lasing Self-Seeded FEL E. Schneidmiller and M. Yurkov ICFA workshop, Arcidosso, Italy, 22.09.2017 Outline Harmonic lasing Harmonic lasing self-seeded (HLSS) FEL Experiments

More information

Linac optimisation for the New Light Source

Linac optimisation for the New Light Source Linac optimisation for the New Light Source NLS source requirements Electron beam requirements for seeded cascade harmonic generation LINAC optimisation (2BC vs 3 BC) CSR issues energy chirp issues jitter

More information

Observation of Coherent Optical Transition Radiation in the LCLS Linac

Observation of Coherent Optical Transition Radiation in the LCLS Linac Observation of Coherent Optical Transition Radiation in the LCLS Linac Henrik Loos, Ron Akre, Franz-Josef Decker, Yuantao Ding, David Dowell, Paul Emma,, Sasha Gilevich, Gregory R. Hays, Philippe Hering,

More information

The CeB6 Electron Gun for the Soft-X-ray FEL Project at SPring-8

The CeB6 Electron Gun for the Soft-X-ray FEL Project at SPring-8 May 25, 2004 DESY, Hamburg, Germany The CeB6 Electron Gun for the Soft-X-ray FEL Project at SPring-8 K. Togawa SPring-8 / RIKEN Harima Institute T. Shintake, H. Baba, T. Inagaki, T. Tanaka SPring-8 / RIKEN

More information

Mechanical Motion Measurement System Design, Initial Results and Experiments with Orbit Feedback

Mechanical Motion Measurement System Design, Initial Results and Experiments with Orbit Feedback Mechanical Motion Measurement System Design, Initial Results and Experiments with Orbit Feedback Workshop on Ambient Ground Motion and Vibration Suppression for Low Emittance Storage Rings 12/11/2017 1

More information

Flexible control of femtosecond pulse duration and separation using an emittance-spoiling foil in x-ray free-electron lasers

Flexible control of femtosecond pulse duration and separation using an emittance-spoiling foil in x-ray free-electron lasers SLAC PUB 16312 June 2015 Flexible control of femtosecond pulse duration and separation using an emittance-spoiling foil in x-ray free-electron lasers Y. Ding 1, C. Behrens 2, R. Coffee 1, F.-J. Decker

More information

Echo-Enabled Harmonic Generation

Echo-Enabled Harmonic Generation Echo-Enabled Harmonic Generation G. Stupakov SLAC NAL, Stanford, CA 94309 IPAC 10, Kyoto, Japan, May 23-28, 2010 1/29 Outline of the talk Generation of microbunching in the beam using the echo effect mechanism

More information

LCLS Beam Diagnostics

LCLS Beam Diagnostics LCLS Beam Diagnostics International Beam Instrumentation Conference 2014 Henrik Loos September 17, 2014 Outline Overview LCLS accelerator diagnostics LCLS-II Charge and beam position Beam profile measurement

More information

David Martin High Precision Beamline Alignment at the ESRF IWAA, Grenoble 3-7 October 2016

David Martin High Precision Beamline Alignment at the ESRF IWAA, Grenoble 3-7 October 2016 David Martin High Precision Beamline Alignment at the ESRF IWAA, Grenoble 3-7 October 2016 OVERVIEW The ESRF has just completed the Phase I Upgrade programme. The Phase I Upgrade programme was centered

More information

LCLS-II Conceptual Design Review. 6 Accelerator

LCLS-II Conceptual Design Review. 6 Accelerator 6 Accelerator Technical Synopsis In order for the Self Amplified Spontaneous Emission (SASE) Free Electron Laser (FEL) to operate in saturation, a high electron peak current with small transverse and longitudinal

More information

MOGA Optimization of LCLS2 Linac

MOGA Optimization of LCLS2 Linac SLAC-PUB-15998 MOGA Optimization of LCLS2 Linac Lanfa Wang, Paul Emma and Tor O. Raubenheimer SLAC National Accelerator Laboratory June 2014 Presented at the FEL 2014 Basel, Switzerland, 25-29 August 2014

More information

Update on Optics Modeling for the ATF Damping Ring at KEK Studies for low vertical emittance

Update on Optics Modeling for the ATF Damping Ring at KEK Studies for low vertical emittance Update on Optics Modeling for the ATF Damping Ring at KEK Studies for low vertical emittance 2009.05.08. K. Kubo, S. Kuroda, T. Okugi (KEK) M.D. Woodley (SLAC), A. Wolski, K. Panagiotidis (U. Liverpool

More information

Part V Undulators for Free Electron Lasers

Part V Undulators for Free Electron Lasers Part V Undulators for Free Electron Lasers Pascal ELLEAUME European Synchrotron Radiation Facility, Grenoble V, 1/22, P. Elleaume, CAS, Brunnen July 2-9, 2003. Oscillator-type Free Electron Laser V, 2/22,

More information

III. CesrTA Configuration and Optics for Ultra-Low Emittance David Rice Cornell Laboratory for Accelerator-Based Sciences and Education

III. CesrTA Configuration and Optics for Ultra-Low Emittance David Rice Cornell Laboratory for Accelerator-Based Sciences and Education III. CesrTA Configuration and Optics for Ultra-Low Emittance David Rice Cornell Laboratory for Accelerator-Based Sciences and Education Introduction Outline CESR Overview CESR Layout Injector Wigglers

More information

Potential use of erhic s ERL for FELs and light sources ERL: Main-stream GeV e - Up-gradable to 20 + GeV e -

Potential use of erhic s ERL for FELs and light sources ERL: Main-stream GeV e - Up-gradable to 20 + GeV e - Potential use of erhic s ERL for FELs and light sources Place for doubling energy linac ERL: Main-stream - 5-10 GeV e - Up-gradable to 20 + GeV e - RHIC Electron cooling Vladimir N. Litvinenko and Ilan

More information

Microbunching Workshop 2010 March 24, 2010, Frascati, Italy. Zhirong Huang

Microbunching Workshop 2010 March 24, 2010, Frascati, Italy. Zhirong Huang Measurements of the LCLS Laser Heater and its impact on the LCLS FEL Performance Z. Huang for the LCLS commissioning team LCLS 1 1 Outline Introduction LCLS setup and measurements Effects on FEL performance

More information

ACCELERATOR LAYOUT AND PHYSICS OF X-RAY FREE-ELECTRON LASERS

ACCELERATOR LAYOUT AND PHYSICS OF X-RAY FREE-ELECTRON LASERS ACCELERATOR LAYOUT AND PHYSICS OF X-RAY FREE-ELECTRON LASERS W. Decking, DESY, Notkestraße 85, 22603 Hamburg, Germany Abstract X-ray Free-Electron Lasers facilities are planned or are already under construction

More information

Matter in Extreme Conditions At LCLS. Gilliss Dyer, December 5, 2018 Fusion Power Associates 39 th Annual Meeting

Matter in Extreme Conditions At LCLS. Gilliss Dyer, December 5, 2018 Fusion Power Associates 39 th Annual Meeting Matter in Extreme Conditions At LCLS Gilliss Dyer, December 5, 2018 Fusion Power Associates 39 th Annual Meeting Switched on in 2009, the Linac Coherent Light Source was the world s first hard x-ray free

More information

4 FEL Physics. Technical Synopsis

4 FEL Physics. Technical Synopsis 4 FEL Physics Technical Synopsis This chapter presents an introduction to the Free Electron Laser (FEL) physics and the general requirements on the electron beam parameters in order to support FEL lasing

More information

Femtosecond and sub-femtosecond x-ray pulses from a SASE-based free-electron laser. Abstract

Femtosecond and sub-femtosecond x-ray pulses from a SASE-based free-electron laser. Abstract SLAC-PUB-12 Femtosecond and sub-femtosecond x-ray pulses from a SASE-based free-electron laser P. Emma, K. Bane, M. Cornacchia, Z. Huang, H. Schlarb, G. Stupakov, and D. Walz Stanford Linear Accelerator

More information

Harmonic Lasing Self-Seeded FEL

Harmonic Lasing Self-Seeded FEL Harmonic Lasing Self-Seeded FEL E. Schneidmiller and M. Yurkov FEL seminar, DESY Hamburg June 21, 2016 In a planar undulator (K ~ 1 or K >1) the odd harmonics can be radiated on-axis (widely used in SR

More information

ERL FOR LOW ENERGY ELECTRON COOLING AT RHIC (LEREC)*

ERL FOR LOW ENERGY ELECTRON COOLING AT RHIC (LEREC)* ERL FOR LOW ENERGY ELECTRON COOLING AT RHIC (LEREC)* J. Kewisch, M. Blaskiewicz, A. Fedotov, D. Kayran, C. Montag, V. Ranjbar Brookhaven National Laboratory, Upton, New York Abstract Low-energy RHIC Electron

More information

Research with Synchrotron Radiation. Part I

Research with Synchrotron Radiation. Part I Research with Synchrotron Radiation Part I Ralf Röhlsberger Generation and properties of synchrotron radiation Radiation sources at DESY Synchrotron Radiation Sources at DESY DORIS III 38 beamlines XFEL

More information

FURTHER UNDERSTANDING THE LCLS INJECTOR EMITTANCE*

FURTHER UNDERSTANDING THE LCLS INJECTOR EMITTANCE* Proceedings of FEL014, Basel, Switzerland FURTHER UNDERSTANDING THE LCLS INJECTOR EMITTANCE* F. Zhou, K. Bane, Y. Ding, Z. Huang, and H. Loos, SLAC, Menlo Park, CA 9405, USA Abstract Coherent optical transition

More information

MaRIE. MaRIE X-Ray Free-Electron Laser Pre-Conceptual Design

MaRIE. MaRIE X-Ray Free-Electron Laser Pre-Conceptual Design Operated by Los Alamos National Security, LLC, for the U.S. Department of Energy MaRIE (Matter-Radiation Interactions in Extremes) MaRIE X-Ray Free-Electron Laser Pre-Conceptual Design B. Carlsten, C.

More information

Novel diagnostics and beam phase space recovery

Novel diagnostics and beam phase space recovery Novel diagnostics and beam phase space recovery C. Emma FACET-II Science Workshop, SLAC October 2017 FACET-II CDR review, Sept. 1-2, Project overview, Yakimenko 1 C. Emma, FACET-II SCIENCE WORKSHOP, Oct.,

More information

Brightness and Coherence of Synchrotron Radiation and Free Electron Lasers. Zhirong Huang SLAC, Stanford University May 13, 2013

Brightness and Coherence of Synchrotron Radiation and Free Electron Lasers. Zhirong Huang SLAC, Stanford University May 13, 2013 Brightness and Coherence of Synchrotron Radiation and Free Electron Lasers Zhirong Huang SLAC, Stanford University May 13, 2013 Introduction GE synchrotron (1946) opened a new era of accelerator-based

More information

Excitements and Challenges for Future Light Sources Based on X-Ray FELs

Excitements and Challenges for Future Light Sources Based on X-Ray FELs Excitements and Challenges for Future Light Sources Based on X-Ray FELs 26th ADVANCED ICFA BEAM DYNAMICS WORKSHOP ON NANOMETRE-SIZE COLLIDING BEAMS Kwang-Je Kim Argonne National Laboratory and The University

More information

SABER Optics. Y. Nosochkov, K. Bane, P. Emma, R. Erickson. SABER Workshop, SLAC, March 15-16, /25

SABER Optics. Y. Nosochkov, K. Bane, P. Emma, R. Erickson. SABER Workshop, SLAC, March 15-16, /25 SABER Optics Y. Nosochkov, K. Bane, P. Emma, R. Erickson SABER Workshop, SLAC, March 15-16, 2006 1/25 Outline White paper optics design Beam tracking for SABER and for the old South Arc Magnet overlap

More information

Energy Stability Update MD Physics Meeting

Energy Stability Update MD Physics Meeting Energy Stability Update MD Physics Meeting Tim Maxwell on behalf of the Stability Performance Program: F.-J. Decker, Andy Benwell, William Colocho, Anatoly Krasnykh, Jeff de Lamare, Jim Lewandowski, Minh

More information

Progress Report on the LCLS XFEL at SLAC

Progress Report on the LCLS XFEL at SLAC Progress Report on the LCLS XFEL at SLAC L F DiMauro 1, J Arthur 2, N Berrah 3, J Bozek 2, J N Galayda 2 and J Hastings 2 1 The Ohio State University, Department of Physics, Columbus, OH 43210 USA 2 Stanford

More information

Commissioning of PETRA III. Klaus Balewski on behalf of the PETRA III Team IPAC 2010, 25 May, 2010

Commissioning of PETRA III. Klaus Balewski on behalf of the PETRA III Team IPAC 2010, 25 May, 2010 Commissioning of PETRA III Klaus Balewski on behalf of the PETRA III Team IPAC 2010, 25 May, 2010 PETRA III Parameters Circumference (m) Energy (GeV) ε x (nm rad) ε y (pm rad) Current (ma) # bunches Straight

More information

GTF Transverse and Longitudinal Emittance Data Analysis Technique * J.F. Schmerge, J.E. Clendenin, D.H. Dowell and S.M. Gierman

GTF Transverse and Longitudinal Emittance Data Analysis Technique * J.F. Schmerge, J.E. Clendenin, D.H. Dowell and S.M. Gierman LCLS-TN-5-19 July 5 GTF Transverse and Longitudinal Emittance Data Analysis Technique * J.F. Schmerge, J.E. Clendenin, D.H. Dowell and S.M. Gierman Abstract The SSRL Gun Test Facility (GTF) was built to

More information

Introduction to the Physics of Tapered Undulator FELs

Introduction to the Physics of Tapered Undulator FELs Introduction to the Physics of Tapered Undulator FELs William M. Fawley Workshop on the Physics and Applications of High Efficiency FELs UCLA 11-13 April 2018 Outline What is undulator tapering and why

More information

X-Band RF Harmonic Compensation for Linear Bunch Compression in the LCLS

X-Band RF Harmonic Compensation for Linear Bunch Compression in the LCLS SLAC-TN-5- LCLS-TN-1-1 November 1,1 X-Band RF Harmonic Compensation for Linear Bunch Compression in the LCLS Paul Emma SLAC November 1, 1 ABSTRACT An X-band th harmonic RF section is used to linearize

More information

Dipole current, bending angle and beam energy in bunch compressors at TTF/VUV-FEL

Dipole current, bending angle and beam energy in bunch compressors at TTF/VUV-FEL Dipole current, bending angle and beam energy in bunch compressors at TTF/VUV-FEL P. Castro August 26, 2004 Abstract We apply a rectangular (hard edge) magnetic model to calculate the trajectory in the

More information

X-band Experience at FEL

X-band Experience at FEL X-band Experience at FERMI@Elettra FEL Gerardo D Auria Elettra - Sincrotrone Trieste GdA_TIARA Workshop, Ångström Laboratory, June 17-19, 2013 1 Outline The FERMI@Elettra FEL project Machine layout and

More information

Tools of Particle Physics I Accelerators

Tools of Particle Physics I Accelerators Tools of Particle Physics I Accelerators W.S. Graves July, 2011 MIT W.S. Graves July, 2011 1.Introduction to Accelerator Physics 2.Three Big Machines Large Hadron Collider (LHC) International Linear Collider

More information

Calculation Of Fields On The Beam Axis Of The Delta Undulator

Calculation Of Fields On The Beam Axis Of The Delta Undulator LCLS-TN-3- Calculation Of Fields On The Beam Axis Of The Delta Undulator Zachary Wolf SLAC December 8, 203 Abstract It is not possible to do Hall probe measurements on the beam axis of the Delta undulator

More information

Nonintercepting ODR Diagnostics for Multi-GeV Electron Beams

Nonintercepting ODR Diagnostics for Multi-GeV Electron Beams Nonintercepting ODR Diagnostics for Multi-GeV Electron Beams Alex H. Lumpkin ASD Diagnostics Group Advanced Photon Source Jefferson Lab CASA Seminar September 28, 2006 OUTLINE Introduction Overview of

More information

Short Introduction to CLIC and CTF3, Technologies for Future Linear Colliders

Short Introduction to CLIC and CTF3, Technologies for Future Linear Colliders Short Introduction to CLIC and CTF3, Technologies for Future Linear Colliders Explanation of the Basic Principles and Goals Visit to the CTF3 Installation Roger Ruber Collider History p p hadron collider

More information

LCLS Accelerator Parameters and Tolerances for Low Charge Operations

LCLS Accelerator Parameters and Tolerances for Low Charge Operations LCLS-TN-99-3 May 3, 1999 LCLS Accelerator Parameters and Tolerances for Low Charge Operations P. Emma SLAC 1 Introduction An option to control the X-ray FEL output power of the LCLS [1] by reducing the

More information

FACET-II Design Update

FACET-II Design Update FACET-II Design Update October 17-19, 2016, SLAC National Accelerator Laboratory Glen White FACET-II CD-2/3A Director s Review, August 9, 2016 Planning for FACET-II as a Community Resource FACET-II Photo

More information

4.2 Photon Beam Line Systems

4.2 Photon Beam Line Systems shielding walls will be ~1-m thick, and the transverse walls will be ~1.5-m thick. Polyethylene will be used to shield neutrons, and additional lead and/or steel will be used for localized shielding as

More information

Undulator radiation from electrons randomly distributed in a bunch

Undulator radiation from electrons randomly distributed in a bunch Undulator radiation from electrons randomly distributed in a bunch Normally z el >> N u 1 Chaotic light Spectral property is the same as that of a single electron /=1/N u Temporal phase space area z ~(/

More information

Greenfield FELs. John Galayda, SLAC Kwang-Je Kim, ANL (Presenter) James Murphy, BNL

Greenfield FELs. John Galayda, SLAC Kwang-Je Kim, ANL (Presenter) James Murphy, BNL Greenfield FELs John Galayda, SLAC Kwang-Je Kim, ANL (Presenter) James Murphy, BNL BESAC Subcommittee on BES 20-year Facility Road Map February 22-24, 2003 What is a Greenfield FEL? High-gain FELs are

More information

THE LCLS-II INJECTOR DESIGN*

THE LCLS-II INJECTOR DESIGN* THE LCLS-II INJECTOR DESIGN* J.F. Schmerge #, A. Brachmann, D. Dowell, A. Fry, R.K. Li, Z. Li, T. Raubenheimer, T. Vecchione, F. Zhou, SLAC, Menlo Park, CA 94025, USA A. Bartnik, I. Bazarov, B. Dunham,

More information

DESY FEL Seminar Progress in Optics Setup / Pt.1

DESY FEL Seminar Progress in Optics Setup / Pt.1 DESY FEL Sem 2019-02-26 / M.Vogt (MFL) J.Zemella (MPY1) / Optics Setup Pt.1 1 DESY FEL Seminar 2019-02-26 Progress in Optics Setup / Pt.1 Mathias Vogt (MFL) & Johann Zemella (MPY1) Reminder: Motivation

More information

Bulk shielding design for the MAX IV facility

Bulk shielding design for the MAX IV facility Bulk shielding design for the MAX IV facility Magnus Lundin 1, Lennart Isaksson 1, Bent Schröder 1 1 Lund University, MAX-lab, P.O. Box 118, SE-221 Lund, Sweden Abstract This paper reports on the design

More information